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Featured researches published by D.D. Carmony.


Physics Letters B | 1998

The role of double parton collisions in soft hadron interactions

T. Alexopoulos; E. W. Anderson; N. Biswas; A. Bujak; D.D. Carmony; A. R. Erwin; L. Gutay; A. Hirsch; C. Hojvat; V.P. Kenney; C.S. Lindsey; J. M. LoSecco; Sergei G. Matinyan; N. Morgan; S. H. Oh; N. Porile; R. P. Scharenberg; B. Stringfellow; M. Thompson; F. Turkot; W.D. Walker; C.H. Wang

Abstract We have examined charged multiplicities arising from p−p and p− p collisions over the range of center of mass energies, s , from 30 GeV to 1800 GeV. Results from Tevatron experiment E735 support the presence of double parton interactions. These processes can be seen to account for a large fraction of the increase in the non single diffraction inelastic cross section from energies of about 200 GeV to 1800 GeV.


Physics Letters B | 1995

Charged particle multiplicity correlations in pp̄ collisions at s=0.3−1.8 TeV

T. Alexopoulos; C. Allen; E. W. Anderson; V. Balamurali; S. Banerjee; P.D. Beery; P. C. Bhat; J.M. Bishop; N. Biswas; A. Bujak; D.D. Carmony; T. Carter; Y. Choi; P. L. Cole; R. DeBonte; V. DeCarlo; A. R. Erwin; C. Findeisen; A. T. Goshaw; L. Gutay; A. Hirsch; C. Hojvat; J. Jennings; V.P. Kenny; C.S. Lindsey; C. Loomis; J. M. LoSecco; T. McMahon; A.P. McManus; N. Morgan

Abstract The correlations between charged particle multiplicitie produced in forward and backward pseudorapidity regions in pp interactions have been measured with a 240 element scintillator hodoscope. The correlation coefficient and the variance of the difference of multiplicities in the two pseudorapidity regions were deterermined for s =0.3−1.8 TeV . These results have been interpreted in terms of a cluster model of particle production.


Physics Letters B | 1977

Inclusive ηp and ηn charged-current neutrino reactions below 6 GeV☆

S.J. Barish; M. Derrick; T. Dombeck; L. Hyman; B. Musgrave; P. Schreiner; R. Singer; M. Szczekowski; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel

Abstract Results are presented of a study of inclusive ηp and ηn interactions from threshold to 6 GeV. The data show a rapid approach to the distributions expected in the naive quark-parton model. The charged-current η deuteron total cross section is fit by the expression σ T ( η d) = (0.76 ± 0.03) × 10 −38 E η cm 2 per GeV per nucleon. For E η > 1.5 GeV, we measure σ T ( η n)/ σ T ( η p) = (2.02 ± 0.23). The distributions in the scaling variables x and y are given and discussed.


Physics Letters B | 2002

Evidence for hadronic deconfinement in p̄–p collisions at 1.8 TeV

T. Alexopoulos; E. W. Anderson; A. Bujak; D.D. Carmony; A. R. Erwin; L. Gutay; A. Hirsch; K. Nelson; N. Porile; S. H. Oh; R. P. Scharenberg; B. Srivastava; B. Stringfellow; F. Turkot; J. Warchol; W.D. Walker

Abstract We have measured deconfined hadronic volumes, 4.4 V 3 , produced by a one-dimensional (1D) expansion. These volumes are directly proportional to the charged particle pseudorapidity densities 6.75 dN c / dη T =179.5±5(syst) MeV. Using Bjorkens 1D model, the hadronization energy density is ϵ F =1.10±0.26(stat) GeV/fm 3 corresponding to an excitation of 24.8±6.2(stat) quark–gluon degrees of freedom.


Physics Letters B | 1995

Charged particle multiplicity correlations in

T. Alexopoulos; J. Warchol; J. Jennings; D.D. Carmony; C. Wang; Swagato Banerjee; P. C. Bhat; S. H. Oh; W.D. Walker; R. P. Scharenberg; P.D. Beery; E. W. Anderson; A. Bujak; D. Reeves; Y. Choi; B. Stringfellow; V.P. Kenney; T. Carter; N. Biswas; N. Porile; L. Gutay; D.K. Wesson; Y. Zhan; C.S. Lindsey; C. Loomis; A. Hirsch; R. DeBonte; C. Hojvat; J.M. Bishop; S.R. Stampke

Abstract The correlations between charged particle multiplicitie produced in forward and backward pseudorapidity regions in pp interactions have been measured with a 240 element scintillator hodoscope. The correlation coefficient and the variance of the difference of multiplicities in the two pseudorapidity regions were deterermined for s =0.3−1.8 TeV . These results have been interpreted in terms of a cluster model of particle production.


Physics Letters B | 1994

p\bar{p}

T. Alexopoulos; C. Allen; E. W. Anderson; V. Balamurali; Swagato Banerjee; P.D. Beery; P. C. Bhat; N. Biswas; A. Bujak; D.D. Carmony; T. Carter; P. L. Cole; Y. Choi; R. DeBonte; V. DeCarlo; A.E. Erwin; C. Findeisen; A. T. Goshaw; L. Gutay; A. Hirsch; C. Hojvat; J. Jennings; V.P. Kenney; C.S. Lindsey; C. Loomis; J. M. LoSecco; T. McMahon; A.P. McManus; N. Morgan; K. Nelson

Transverse momentum spectra of charged particles produced within the pseudo-rapidity range of η= − 0.36 to + 1.0 have been measured in pp collisions at √s=0.3, 0.54, 1.0, and 1.8 TeV. The spectra are presented as a function of event charged multiplicity within the range −3.25<η<3.25. We found that the slope in the low pt region is independent of center-of-mass energy and multiplicity while the slope at the high pt region shows a strong energy and multiplicity dependence.


Physics Letters B | 1979

collisions at

M. Derrick; A. Fridman; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen

Abstract Using new ν p charged-current data from the Fermilab 15 foot hydrogen bubble chamber, some properties of the ν -induced hadronic jets are studied. The angular size of the jets is measured and compared with results from e + e − annihilation. The jets in the two processes are found to be quite similar in terms of the variables sphericity, thrust, and energy flow.


Physics Letters B | 1980

\sqrt{s}

M. Derrick; E. Fernandez; L. Hyman; G. Levman; D. Koetke; B. Musgrave; P. Schreiner; R. Singer; S. Toaff; S.J. Barish; A. Engler; R.W. Kraemer; B.J. Stacey; M. Tabak; R. Ammar; D. Coppage; D. Day; R. Davis; N. Kwak; R. Stump; V. E. Barnes; D.D. Carmony; A. F. Garfinkel; C. Kennedy; G.M. Radecky

Abstract We have measured the excitation function for the neutral current process νn→νpπ− as a function of neutrino energy. Our data give a cross section ratio R=σ(νpπ−)/σ(μ−pπ+)=0.11±0.022 over the energy interval (0.3⩽E ν⩽1.5)GeV. This measurement of single-pion production in a kinematically defined reaction is the first to use a deuterium target. The R value, as well as other characteristics of the data, agrees with the Adler model for single-pion production via the neutral current and gives a value of sin2θw=0.26±0.09.


Physics Letters B | 1980

= 0.3-TeV to 1.8-TeV

M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen

Abstract Using data from the Fermilab 15 ft hydrogen bubble chamber, we have studied inclusive ϱ0 production in antineutrino-proton charged-current interactions. We measure (0.21 ± 0.03) ϱ0/event, corresponding to ϱ0/π−=0.12 ± 0.02. As a function of Q2 and for hadronic masses above a threshold region, the ϱ0/π− ratio shows little variation. At least 50% of the ϱ0s are consistent with coming from the current fragmentation region. The results agree reasonably well with the predictions of the quark fragmentation model of Feynman and field.


Physics Letters B | 1980

Multiplicity dependence of transverse momentum spectra of centrally produced hadrons in pp collisions at 0.3, 0.54, 0.9, and 1.8 TeV center of mass energy

M. Derrick; P. Gregory; F. LoPinto; B. Musgrave; J. L. Schlereth; P. Schreiner; R. Singer; S.J. Barish; R. Brock; A. Engler; T. Kikuchi; R.W. Kraemer; F. Messing; B.J. Stacey; M. Tabak; V. E. Barnes; D.D. Carmony; E. Fernandez; A. F. Garfinkel; A. T. Laasanen

Abstract The hadronic system produced in charged-current antineutrino interactions is used to study fragmentation of the d-quark. Some problems encountered in defining the current quark fragments are discussed. The properties of the fragmentation function are in good agreement with the expectations of the naive quark-parton model and, in particular, at the present level of statistics we find no need for either a Q 2 -or an x BJ -dependence.

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B. Musgrave

Argonne National Laboratory

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P. Schreiner

Argonne National Laboratory

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R. Singer

Argonne National Laboratory

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S.J. Barish

Argonne National Laboratory

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N. Biswas

University of Notre Dame

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